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作 者:郭竞渊 唐强[1] 唐桦明 张纯祥[1] 罗达玲[1] 刘小伟[1]
机构地区:[1]中山大学物理学院,广州510275
出 处:《物理学报》2017年第10期302-308,共7页Acta Physica Sinica
基 金:国家自然科学基金(批准号:11375278);广东省自然科学基金(批准号:2016A030313276);广州市科技计划项目(批准号:20160701168)资助的课题~~
摘 要:采用高温固相法合成了LiMgPO_4:Tm,Tb粉末样品,测定了热释光陷阱参数激发能E和频率因子s.用脉冲退火和多次退火方法研究了其光释光陷阱参数E和s,并与用多速法得到的热释光的结果进行了比较.对不同β射线剂量照射的样品发光曲线的研究表明,300°C高温峰属于一级动力学发光峰.通过对热释光和光释光陷阱的相关性研究表明,经200°C预热的热释光信号(对应于300°C高温峰)和光释光信号很有可能来自于同一深度的陷阱.In recent years, the preparation and luminescent properties of LiMgPO4 as a matrix have received much attention, but most of the studies are limited to the trap parameters of thermoluminescence (TL), which do not involve the trap parameters of optical stimulated luminescence (OSL). In this paper, LiMgPO4:Tm, Tb powder samples are synthesized by solid-state reaction at high temperature. All the experiments reported here are measured by Riso TL/OSL-15-B/C reader after being irradiated by beta-rays. The TL glow curves obtained show that the high temperature peak at 300℃ belongs to the first-order kinetic peak because the peak temperature does not change as irradiation dose increases. Based on the first-order kinetics, the TL trap depth E = 1.72 eV and the frequency factor s= 3.97× 1014 are determined by the methods of various heating rates. However, LiMgPO4:Tm, Tb is also an OSL material, the analysis of its OSL trap kinetic parameters would help to understand the OSL mechanism and to know the relationship between TL and OSL traps. The pulse annealing method is suitable for OSL trap parameter analysis. For low sensitivity samples, the fluctuation of the pulse annealing method is relatively large. And this method only records the OSL signal of fast decay component, which is suitable for measuring the samples with high sensitivity and fast fading OSL signals. In order to study the OSL signal of slow decay component, the multiple annealing method is proposed based on the pulse annealing method. The multiple annealing procedure is as follows. Firstly, the sample is annealed from room temperature to 500℃ which lasts 30 s. The heating rate is 5℃/s. Secondly, the sample is irradiated with 90Sr beta radiation doses of 1 Gy. Thirdly, the sample is preheated to 150℃ with a heating rate of 0.2 ℃/s. And then OSL measurement lasts 500 s after cooling to room temperature. The above steps are repeated in preheating temperature steps of 10℃. Four repetitive measurements are made for each preheating rate. T
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